International Patent Publication
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International Patent Publication
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Abstract A process (international patent publication n° WO 2009/125444 A1) capable of producing large amounts of energy by a nuclear fusion process between nickel and hidrogen, occurring below 1000 K, is described. Experimental values of the ratios between output and input energies obtained in a certain number of experiments are reported. The occurrence of the effect is justified on the basis of existing experimental and theoretical results. Measurements performed during the experiments allow to exclude neutron and gamma rays emissions. Sergio Focardi
Introduction It is well known that in chemical reactions, and more specifically in processes used to obtain energy, as for example oil, gas and carbon combustion, only some electronVolts (eV) can be obtained for every couple of atoms involved. This depends on the fact that binding energies of external atomic electrons are in the eV range. On the other hand, in nuclear transformations, the energy quantities that can be absorbed or released are of the order of mega-electronVolts (MeV) for every couple of nuclei involved in the process. As a consequence, for every given amount of energy obtained, the mass to be transformed by a nuclear process is about a millionth of that necessary for a combustion. Experimental results In this paper we report the results obtained with a process and apparatus not described here in detail and protected by patent in 90 countries, consisting of a system whose heat output is up to hundred times the electric energy input. As a consequence, the principle of the conservation of energy ensures that processes involving other energy forms are occurring in our apparatus. The system on which we operate consists of Ni, in H atmosphere and in the presence of additives placed in a sealed container and heated by a current passing through a resistor. The maximum temperature value can be set to a wide range of values and an external meter allows us to measure the electric energy input. The container is in thermal contact with an external tank full of water and thermally insulated in order to minimize outside heat exchanges. As consequence of the energy production of the system, water boils and the water pipe is under pressure. The steam pressure cannot exceed a limit, whose value can be changed in the range 3-6 bar, because of the opening of a valve. When the valve opens, new water, whose amount is measured by a meter, enters from the supply. These data allow us to calculate the power produced by our system. Theoretical interpretation Proton capture by Nickel nuclei obviously requires the overcoming of an electrostatic potential barrier which opposes the process. For Ni58(the more abundant Nickel isotope), the maximum potential energy Vmax occurs at a distance R between Ni and proton nuclei centers equal to the sum of their radii, that is R ≈ 6,1 fm. The Vmax value is given (in CGS units) by the expression Vmax=Zeˆ2/R , where Zeˆ2 is the product of the two nuclear charges: it results in Vmax=1,06*10ˆ-5erg=662 keV. The proton kinetic energy Ke can be easily estimated by the relation Ke=1/2 mvˆ2=3/2 kT, where k is Boltzmann’s constant and T is the temperature measured in Kelvin: also on assuming T=1000 K, Ke is only ≈0,9 eV. According to classical physics, a particle having an energy of about 1 eV cannot overcome such a very high potential barrier. Such an opportunity, in principle, is given by the quantum mechanical tunnel e¤ect: in this case, the incoming particle can penetrate into the nucleus by getting through the potential barrier. The tunneling probability of a single particle colliding with an atomic target has been calculated by Gamow [9]. As shown by Evans [10], such a probability can be approximated as Conclusions In conclusion, our process and apparatus is the first and unique system, existing today, able to obtain energy from nuclear fusion reactions; furthermore, because the ingredients are Nickel and water (to obtain Hydrogen), this is an endless energy source for the planet, without emissions in atmosphere. Sergio Focardi Bibliography [1] R.D. Evans, The Atomic Nucleus, Mcgraw-Hill, New York 1955, pag.297. [2] nuclear mass values have been taken by Table of Isotopes, eight edition, march 1996, Wiley Interscience . [3] G. A. Cowan, “A Natural Fission Reactor,” Scienti.c American, 235:36, (1976). [4] A.P. Arya, Elementary Modern Physics, Addison-Wesley publishing company, Reading Massachussets (1974), pag. 399. |
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